
defining the incompressibility \(K_0\equiv 9\rho _0^2\mathrm {d}^2E_0(\rho )/\mathrm {d}\rho ^2|_{\rho =\rho _0}\)  and skewness \(J_0\equiv 27\rho _0^3\mathrm {d}^3E_0(\rho )/\mathrm {d}\rho ^3|_{\rho =\rho _0}\)  of the SNM, the slope coefficient \(L\equiv 3\rho _0\mathrm {d}E_{\mathrm {sym}}(\rho )/\mathrm {d}\rho |_{\rho =\rho _0}\) , the curvature coefficient \(K_{\mathrm {sym}}\equiv 9\rho _0^2\mathrm {d}^2E_{\mathrm {sym}}(\rho )/\mathrm {d}\rho ^2|_{\rho =\rho _0}\)  and the skewness coefficient \(J_{\mathrm {sym}}\equiv 27\rho _0^3\mathrm {d}^3E_{\mathrm {sym}}(\rho )/\mathrm {d}\rho ^3|_{\rho =\rho _0}\)  of the symmetry energy, etc., here the dimensionless quantity \(\chi \)  is defined as \(\chi =(\rho -\rho _0)/3\rho _0\) .
The EOS of ANM provides an important and basic input for various applications in both nuclear physics and astrophysics [1]}, [2]}, [3]}, [4]}, [5]}, [6]}, [7]}, [8]}, [9]}.
